TW201249564A - Ferromagnetic granular powder and method for manufacturing same, as well as anisotropic magnet, bonded magnet, and pressed-powder magnet - Google Patents
Ferromagnetic granular powder and method for manufacturing same, as well as anisotropic magnet, bonded magnet, and pressed-powder magnet Download PDFInfo
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Abstract
Description
201249564 六、發明說明: 【發明所屬之技術領域】 本發明係有關一種粒子核爲FeI6N2,外殻被由非常薄 的FeO而成的氧化膜所被覆之強磁性粒子粉末及其製造 法。並提供使用該強磁性粒子粉末之異向性磁石、黏結磁 石及壓粉磁石。 【先前技術】 現在,油電混合汽車或電動車、冷氣機或洗衣機等之 家電等身邊的能量·轉矩使用Nd-Fe-B系磁性粉末·成形 體作爲必要的馬達用磁石。然而,目前作爲Nd-Fe-B系磁 石材料之磁石的理論臨界値。 另外,價格便宜的原料成本或同位素元素含有率低等 誘人的稀土類元素原料的輸入大都偏於中國,即”中國風 險”的大問題。因此,著重於不含稀土類元素之Fe16N2等 之Fe-N系化合物。 於Fe-N系化合物中,已知有a”-Fe16N2係使固溶氮 之馬氏體或純粒鐵長時間進行混練時晶出的-準安定化合物 。該a"-Fel6N2之結晶爲bet構造,期待作爲具有大的飽 和磁化之巨大磁性物質。然而,極少有使準安定化合物之 該化合物爲經離析的粉末予以化學合成的報告。2012. The invention relates to a ferromagnetic particle powder in which a particle core is FeI6N2 and an outer shell is coated with an oxide film made of very thin FeO, and a method for producing the same. An anisotropic magnet, a bonded magnet, and a powdered magnet using the ferromagnetic particle powder are also provided. [Prior Art] Now, the Nd-Fe-B-based magnetic powder and molded body are used as the necessary magnet for the electric energy and torque of the electric-electric hybrid car, the electric vehicle such as an electric car, an air conditioner, or a washing machine. However, the current theoretical criticality of magnets as Nd-Fe-B based magnet materials. In addition, the low cost of raw materials or the low content of isotopic elements, such as the attractive input of rare earth element materials, are mostly biased towards China, which is a big problem of “China risk”. Therefore, an emphasis is placed on Fe-N compounds such as Fe16N2 which do not contain a rare earth element. Among the Fe-N-based compounds, a--Fe16N2 is a quasi-stabilized compound which crystallizes solid solution nitrogen martensite or pure granular iron for a long period of time. The crystal of the a"-Fel6N2 is bet The structure is expected to be a large magnetic substance having a large saturation magnetization. However, there is very little report that the compound of the quasi-stabilized compound is chemically synthesized as an isolated powder.
直至目前,爲製得a”-Fe16N2單相時,·試行蒸鍍法、 MBE法(分子線定向附晶生長法)、離子注入法、濺鑛法、 銨氮化法等之方法。然而,不易生成較爲安定的γ'-F^N 201249564 或ε-Fq〜:)N,同時會引起如馬氏體(a,.Fe)或純粒鐵(a_Fe) 之金屬的共晶,以離析製造a"_Fei6N2單—化合物。可得 部分a"-Fei6N2單一化合物作爲薄膜,惟薄膜適用於磁性 材料中有限,無法展開更爲寬廣的用途。 有關oT-Fe^N2之已知技術,提案有下述技術。 [習知技術文獻] [專利文獻] 專利文獻1 :日本特開平11-340023號公報 專利文獻2 :日本特開2000-277311號公報 專利文獻3 :日本特開2009-84115號公報 專利文獻4 :日本特開2008-108943號公報 專利文獻5:日本特開2008-103510號公報 專利文獻6:曰本特開2007-335592號公報 專利文獻7 :日本特開2007-258427號公報 專利文獻8:曰本特開2007-134614號公報 專利文獻9:日本特開2007-36027號公報 專利文獻10 :日本2009-249682號公報 [非專利文獻] 非專利文獻 1 : M. Takahashi,H. Shoji,H.Up to now, in order to obtain a single phase of a"-Fe16N2, a method such as a vapor deposition method, a MBE method (molecular line oriented epitaxial growth method), an ion implantation method, a sputtering method, an ammonium nitridation method, etc. has been tried. It is not easy to generate relatively stable γ'-F^N 201249564 or ε-Fq~:)N, and at the same time cause eutectic of metal such as martensite (a, .Fe) or pure iron (a_Fe) to isolate Manufacture of a "_Fei6N2 single-compound. Partial a"-Fei6N2 single compound can be obtained as a film, but the film is suitable for magnetic materials and can not be expanded for wider use. For the known technology of oT-Fe^N2, the proposal has [Patent Document] [Patent Document] [Patent Document 1] Japanese Patent Laid-Open Publication No. Hei. No. Hei. No. Hei. No. Hei. No. 2000-277311. Patent Document 4: JP-A-2008-108943, Patent Document 5: JP-A-2008-103510, JP-A-2007-335592, JP-A-2007-335592, JP-A-2007-258427, JP-A-2007-258427 Document 8: 曰本特开2007-134614号 Patent Document 9: Day Laid-Open Publication No. 2007-36027 Patent Document 10: Japanese Patent Publication No. 2009-249682 [Patent Document] Patent Document 1:. M. Takahashi, H Shoji, H.
Takahashi, H. Nashi, χ Wakiyama, Μ. Doi, and Μ.Takahashi, H. Nashi, χ Wakiyama, Μ. Doi, and Μ.
Matsui,J. Appl. Phys.,ν〇1· 76,pp.6642-6647,1 994。 非專利文獻 2: Y. Takahashi, Μ. Katou, Η. Shoji, 201249564 and M. Takahashi, J. Magn. Magn. Mater., Vol.232, p. 18 -26,2001 ° 【發明內容】 於上述專利文獻1〜10及非專利文獻1及2記載的技 術,無法說爲充分。 換言之,於專利文獻1中,雖記載使存在表面氧化被 膜之鐵粒子予以還原處理後,進行氮化處理,製得Fe16N2 ’惟沒有考慮提高最大能量積。而且,氮化反應需經過長 時間(例如3〜1 0日)者,無法說可工業化。 另外,於專利文獻2中,雖記載使氧化鐵粉末予以還 原處理’生成金屬鐵粉末,使所得的金屬鐵粉末進行氮化 處理’製得Fe ! 6N2,爲使用作爲磁性記錄媒體用磁性粒子 粉末者,無法說可適用作爲具有高的最大能量積BHmax之 硬磁性材料。 此外,於專利文獻3〜9中,雖記載改成純粒鐵之磁 性記錄材料用之極大磁性物質,惟無法製得a"-Fe16N2單 相,生成作爲混相之如更安定的Y'-Fe4N或s-Fe2〜3N、馬 氏體(a'-Fe)或純粒鐵(α-Fe)之金屬。 而且,於專利文獻1 〇中,沒有詳細討論添加元素爲 必須及有關其必要性,同時有關所得的生成物之磁性特性 ,無法說適合使用作爲具有高的最大能量積ΒΗη^χ之硬磁 性材料者。 於非專利文獻1〜2中,可成功地製得薄膜之a"- 201249564Matsui, J. Appl. Phys., ν〇1·76, pp.6642-6647, 1 994. Non-Patent Document 2: Y. Takahashi, Μ. Katou, Η. Shoji, 201249564 and M. Takahashi, J. Magn. Magn. Mater., Vol. 232, p. 18-26, 2001 ° [Summary of the Invention] The techniques described in Patent Documents 1 to 10 and Non-Patent Documents 1 and 2 cannot be said to be sufficient. In other words, in Patent Document 1, it is described that after the iron particles having the surface oxide film are subjected to reduction treatment, nitriding treatment is performed to obtain Fe16N2', but the maximum energy product is not considered to be increased. Moreover, the nitriding reaction takes a long time (for example, 3 to 10 days), and it cannot be said that it can be industrialized. Further, in Patent Document 2, it is described that the iron oxide powder is subjected to reduction treatment to form a metal iron powder, and the obtained metal iron powder is subjected to nitriding treatment to obtain Fe 6 6N2, which is used as a magnetic particle powder for a magnetic recording medium. It cannot be said that it is applicable as a hard magnetic material having a high maximum energy product BHmax. Further, in Patent Documents 3 to 9, although a very large magnetic substance for a magnetic recording material of pure granular iron is described, a single phase of a"-Fe16N2 cannot be obtained, and a more stable Y'-Fe4N is produced as a mixed phase. Or a metal of s-Fe2~3N, martensite (a'-Fe) or pure iron (α-Fe). Further, in Patent Document 1 ,, the addition of an element is not necessary in detail and its necessity, and the magnetic properties of the resultant product cannot be said to be suitable for use as a hard magnetic material having a high maximum energy product. By. In Non-Patent Documents 1 to 2, a film can be successfully produced a"- 201249564
Fe i όΝ2單相’惟薄膜之適用受到限制,無法展開更爲廣泛 的用途。而且’作爲一般的磁性材料時,在生產性或經濟 性上會有問題。 因此,本發明係以提供一種覆蓋於高純度且極薄的 FeO上之Fe^N2強磁性粒子粉末' 該強磁性粒子粉末之 製造方法、使用該粉末之異向性磁石、黏結磁石及壓粉磁 石爲目的。 可藉由下述之本發明予以解決。 換言之’本發明係有關一種強磁性粒子粉末,其特徵 爲以由穆斯堡爾光譜之Fe i 6N2化合物相爲8 0%以上之比 例所構成的強磁性粒子粉末’該強磁性粒子在粒子外殻中 存在FeO,同時FeO之膜厚爲5nm以下(本發明1)。 本發明係有關本發明1之強磁性粒子粉末其表面之 Fe◦的體積分率,於FeO體積/粒子全體體積中爲25%以 下(本發明2)。 本發明係有關本發明1或2記載之強磁性粒子粉末, 其中保磁力 Hc爲1 .5k0e以上,5K之飽和磁化as爲 1 50emu/g以上(本發明3) » 此外,本發明係有關本發明1〜3中任一項記載之強 磁性粒子粉末,其中由格子定數所求得的氮化率爲8〜 1 3 m ο 1 % (本發明 4)。 另外,本發明係有關本發明1〜4中任一項記載之強 磁性粒子粉末之製造法,其中 BET比表面積爲5〜 40m2/g(本發明 5)» 201249564 而且,本發明係有關本發明1〜5中任一項記載之強 磁性粒子粉末之製造法,其中使用平均長軸直徑爲40〜 5000nm、縱橫比(長軸直徑/短軸直徑)爲1〜200之氧化鐵 或氧基氫氧化鐵爲出發原料,進行凝聚粒子分散處理使 D:5 0爲40μιη以下、D90爲150μηι以下,再使通過250μπι 以下篩網的鐵化合物粒子粉末在160〜42(TC下進行氫還原 ,且在130〜17(TC下進行氮化處理(本發明6)。 此外,本發明係有關一種異向性磁石,其係由本發明 1〜5中任一項記載之強磁性粒子粉末所形成(本發明7)。 另外,本發明係有關一種黏結磁石,其係含有本發明 1〜5中任一項記載之強磁性粒子粉末(本發明8)。 而且,本發明係有關一種壓粉磁石,其係含有本發明 1〜5中任一項記載之強磁性粒子粉末(本發明9) » [發明效果] 本發明之強磁性粒子粉末,適合作爲極高純度且安定 的磁性材料。 而且,本發明之強磁性粒子粉末之製造法,由於可容 易製得高純度且安定的Fel6N2粒子粉末,適合作爲強磁 性粒子粉末之製造法。 [爲實施發明之最佳形態] 首先,說明有關本發明之強磁性粒子粉末. 本發明之強磁性粒子粉末係以由穆斯堡爾光譜之 -9- 201249564The use of Fe i όΝ2 single-phase ** film is limited and cannot be used for a wider range of applications. Moreover, when it is a general magnetic material, there is a problem in productivity or economy. Accordingly, the present invention provides a Fe^N2 ferromagnetic particle powder coated on a high-purity and extremely thin FeO, a method for producing the ferromagnetic particle powder, an anisotropic magnet using the powder, a bonded magnet, and a powder Magnet for the purpose. This can be solved by the present invention described below. In other words, the present invention relates to a ferromagnetic particle powder characterized in that a ferromagnetic particle powder composed of a ratio of a Fe i 6N 2 compound phase of a Mossbauer spectrum of 80% or more 'the ferromagnetic particle is outside the particle FeO is present in the shell, and the film thickness of FeO is 5 nm or less (Invention 1). The present invention relates to a ferromagnetic particle powder according to the invention 1 having a volume fraction of Fe 表面 on the surface thereof, which is 25% or less in the FeO volume/particle total volume (Invention 2). The present invention relates to the ferromagnetic particle powder according to the invention 1 or 2, wherein the coercive force Hc is 1.5 k0e or more, and the saturation magnetization as of 5 K is 1 50 emu/g or more (Invention 3). Further, the present invention relates to the present invention. The ferromagnetic particle powder according to any one of Inventions 1 to 3, wherein the nitridation ratio determined by the lattice number is 8 to 13 m ο 1 % (Invention 4). Further, the present invention relates to a method for producing a ferromagnetic particle powder according to any one of the present invention, wherein a BET specific surface area is 5 to 40 m 2 /g (Invention 5)» 201249564 Further, the present invention relates to the present invention. The method for producing a ferromagnetic particle powder according to any one of 1 to 5, wherein an iron oxide or an oxyhydrogen having an average major axis diameter of 40 to 5000 nm and an aspect ratio (long axis diameter/minor axis diameter) of 1 to 200 is used. The iron oxide is used as a starting material, and the agglomerated particle dispersion treatment is carried out so that D:50 is 40 μm or less, and D90 is 150 μm or less, and the iron compound particle powder passing through a sieve of 250 μm or less is subjected to hydrogen reduction at 160 to 42 (TC). The present invention relates to an anisotropic magnet formed by the ferromagnetic particle powder according to any one of the inventions 1 to 5 (the present invention). Further, the present invention relates to a bonded magnet comprising the ferromagnetic particle powder according to any one of the present inventions 1 to 5 (Invention 8). Further, the present invention relates to a powder magnetic magnet, which is a system Containing the present invention 1 to 5 The ferromagnetic particle powder of the present invention is suitable as a magnetic material of extremely high purity and stability. Moreover, the production of the ferromagnetic particle powder of the present invention is also suitable as a magnetic material of extremely high purity and stability. In the method, a high-purity and stable Fel6N2 particle powder can be easily obtained, which is suitable as a method for producing a ferromagnetic particle powder. [Best Mode for Carrying Out the Invention] First, a ferromagnetic particle powder according to the present invention will be described. Strong magnetic particle powder is used by Mössbauer -9-201249564
Fe16N2化合物相爲80%以上所構成》穆斯堡爾光譜爲生成 Fe16N2時,被確認內部磁場爲330k〇e以上之鐵側之波峰 ,特別是特徵在3 95 kOe附近出現波峰。 —般而言,他相多時,由於出現作爲軟性磁石之特性 強,不適合作爲強磁性黏結磁石材料。而且,本發明可發 揮作爲強磁性黏結磁石材料之充分特性。 強磁性粒子粉末係粒子核爲Fe16N2、粒子外殼上存在 FeO者,自粒子核朝向外殼之Fe16N2/FeO的簡單構造所 構成。Fel6N2與FeO局部規整性鍵結,以結晶學連績較 佳。該外殼之氧化膜中不含 Fe304或 Fe203、α-Fe。 Fe16N2粒子爲低純度時,亦含有此等之雜質,惟藉由高純 度化形成僅FeO。FeO之膜厚爲5nm以下,較佳者爲4nm 以下。伴隨Fe16N2之高純度化,該FeO之膜厚變薄。FeO 膜厚沒有特別的限制,愈薄時,爲提高粒子中所含的 Fei6N2體積分率愈佳。FeO之膜厚的下限値約爲0.5nm。 本發明之強磁性粒子粉末表面之FeO的體積分率, 於FeO體積/粒子全體積中以25%以下較佳。藉由使 Fel6N2高純度化,減少FeO之體積分率。較佳的FeO之 體積分率爲23%以下,更佳者爲3〜20°/«^ 本發明之強磁性粒子粉末,以保磁力H。爲1 .5kOe以 上、5K之飽和磁化as爲150emu/g以上較佳。飽和磁化 値as及保磁力He未達前述範圍時,無法說作爲硬磁性材 料之磁性特性充分。較佳的保磁力He爲1.6kOe以上,飽 和磁化値σ s爲1 8 0 e m u / g以上。 -10- 201249564 本發明之強磁性粒子粉末,以藉由格子定數所求取的 氮化率爲8〜13mol%較佳。藉由Fe16N2之化學組成式求 得的11」111〇1%最適合》較佳的氮化率爲8.5〜12.5111〇1%, 更佳者爲9.0〜12mol%。 本發明之強磁性粒子粉末之BET比表面積,以5.0〜 40m2/g較佳。BET比表面積未達5m2/g時,氮化率變低, 結果之Fe16N2生成率降低,且無法製得企求的保磁力或 飽和磁化。超過40m2/g時,無法得到企求的飽和磁化値 。較佳的BET比表面積爲5.5〜38m2/g,更佳者爲6.0〜 3 5 m2/g。 其次,說明有關本發明之強磁性粒子粉末之製造法。 本發明之強磁性粒子粉末,係使用平均長軸直徑爲 40〜5000nm、縱橫比(長軸直徑/短軸直徑)爲1〜200之氧 化鐵或氧基氫氧化鐵爲出發原料,進行凝聚粒子分散處理 使D50爲40μιη以下、D90爲150μπι以下,再使通過 25〇μπι以下篩網的鐵化合物粒子粉末在160〜420°C下進行 氫還原,且在130〜17(TC下進行氮化處理。存在粒子外殼 之FeO,藉由於氮化處理後,使僅粒子表面界面之氮氣被 除去的鐵金屬部分氧化而產生者。 於本發明中,係使用平均長軸直徑爲40〜5000nm、 縱橫比(長軸直徑/短軸直徑)爲1〜200之氧化鐵或氧基氫 氧化鐵爲出發原料。The composition of the Fe16N2 compound phase is 80% or more. When the Mossbauer spectrum is Fe16N2, it is confirmed that the internal magnetic field is a peak of the iron side of 330 k〇e or more, and particularly, a peak appears in the vicinity of 3 95 kOe. In general, when he is a long time, it is not suitable as a ferromagnetic bonded magnet material because of its strong properties as a soft magnet. Moreover, the present invention can exert sufficient characteristics as a ferromagnetic bonded magnet material. The ferromagnetic particle powder-based particle core is Fe16N2, and FeO exists on the outer shell of the particle, and the simple structure of Fe16N2/FeO from the particle core toward the outer shell is formed. Fel6N2 and FeO are locally bonded, and the crystallography is better. The oxide film of the outer casing does not contain Fe304 or Fe203 or α-Fe. When the Fe16N2 particles are of low purity, they also contain such impurities, but only FeO is formed by high purity. The film thickness of FeO is 5 nm or less, preferably 4 nm or less. With the high purity of Fe16N2, the film thickness of the FeO becomes thin. The FeO film thickness is not particularly limited, and the thinner the film, the better the volume fraction of Fei6N2 contained in the particles is. The lower limit 膜 of the film thickness of FeO is about 0.5 nm. The volume fraction of FeO on the surface of the ferromagnetic particle powder of the present invention is preferably 25% or less in the FeO volume/particle total volume. By increasing the purity of Fel6N2, the volume fraction of FeO is reduced. The preferred FeO has a volume fraction of 23% or less, more preferably 3 to 20 °/«. The ferromagnetic particle powder of the present invention has a coercive force H. The saturation magnetization as of 1.5 kOe or more and 5 K is preferably 150 emu/g or more. When the saturation magnetization 値as and the coercive force He do not reach the above range, it cannot be said that the magnetic properties of the hard magnetic material are sufficient. The preferred coercive force He is 1.6 kOe or more, and the saturation magnetization 値 σ s is 1 800 n m u / g or more. -10- 201249564 The ferromagnetic particle powder of the present invention preferably has a nitridation ratio of 8 to 13 mol% as determined by a lattice number. The preferred nitridation ratio of 11"111〇1% obtained by the chemical composition formula of Fe16N2 is 8.5 to 12.5111 〇 1%, more preferably 9.0 to 12 mol%. The BET specific surface area of the ferromagnetic particle powder of the present invention is preferably 5.0 to 40 m 2 /g. When the BET specific surface area is less than 5 m2/g, the nitriding rate becomes low, and as a result, the Fe16N2 formation rate is lowered, and the desired coercive force or saturation magnetization cannot be obtained. When it exceeds 40 m2/g, the desired saturation magnetization 无法 cannot be obtained. A preferred BET specific surface area is 5.5 to 38 m 2 /g, and more preferably 6.0 to 3 5 m 2 /g. Next, a method of producing the ferromagnetic particle powder of the present invention will be described. The ferromagnetic particle powder of the present invention is obtained by using iron oxide or iron oxyhydroxide having an average major axis diameter of 40 to 5000 nm and an aspect ratio (long axis diameter/minor axis diameter) of 1 to 200 as a starting material. The dispersion treatment is such that D50 is 40 μm or less and D90 is 150 μm or less, and the iron compound particle powder passing through a sieve of 25 μm or less is subjected to hydrogen reduction at 160 to 420 ° C, and nitriding treatment is performed at 130 to 17 (TC). The FeO in the outer shell of the particle is produced by oxidizing the iron metal portion from which the nitrogen at the surface of the particle surface is removed after the nitriding treatment. In the present invention, the average major axis diameter is 40 to 5000 nm, and the aspect ratio is used. (Long axis diameter / short axis diameter) is 1 to 200 iron oxide or iron oxyhydroxide as a starting material.
出發原料之氧化鐵或氧基氫氧化鐵,沒有特別的限制 ’例如磁鐵礦、Y-Fe2〇3 ' a-Fe2〇3 ' a-FeOOH ' β-FeOOH -11 - 201249564 、γ-FeOOH、FeO等。而且,即使出發原料爲單相時,亦 可含有雜質,亦可含有主相以外之氧化鐵或氧基氫氧化鐵 作爲雜質》 出發原料之氧化鐵或氧基氫氧化鐵之粒子形狀沒有特 別的限制可爲針狀、粒狀、紡錘狀、直方體狀、球狀等之 任一種。 本發明之鐵化合物粒子粉末之縱橫比(長軸直徑/短軸 直徑),以1.0〜200較佳。超過該範圍時,不易製得目的 之以由穆斯堡爾光譜之Fe16N2化合物相爲80%以上所構 成的強磁性粒子粉末。較佳的縱橫比爲1.0〜190,更佳者 爲 1.0〜180 。 出發原料之鐵化合物粒子粉末的BET比表面積,以 20〜25 0m2/g較佳。BET比表面積未達20m2/g時,不易進 行氮化處理,無法製得目的之由穆斯堡爾光譜之Fe16N2 化合物相爲80%以上所構成的強磁性粒子粉末。BET比表 面積超過250m2/g時,由於引起過剩的氮化,故無法製得 由穆斯堡爾光譜之Fe16N2化合物相爲80%以上所構成的 強磁性粒子粉末。較佳的BET比表面積爲30〜200m2/g, 更佳者爲35〜1 80m2/g » 於本發明中出發原料之氧化鐵或氧基氫氧化鐵之凝聚 粒子直徑,以控制於D50爲40μηι以下、D90爲150μηι以 下較佳。由於出發原料使用粉末,~般而言凝聚粒子直徑 相當大。使其凝聚粒子直徑小的方法,沒有特別的限制, 例如可在醇化合物、酮化合物或甲苯、己烷、四氯化碳、 -12- 201249564 環己烷等之有機溶劑存在下,進行球磨或行星球磨、濕式; 粉碎’且進行噴射磨粉碎。較佳者D50爲35μιη以下、 D90爲125μιη以下,更佳者D50爲30μιη以下、D90爲 1 0 0 μ m以下。 本發明之鐵化合物粒子粉末,以於熱處理前預先通過 2 5 0μιη以下之篩網爲宜。超過2 5 0μιη之篩網尺寸,不易 製得可發揮企求的磁性特性之強磁性粒子粉末。較佳者爲 236μηι 以下。 對氧基氫氧化鐵而言,視其所需進行脫水處理時,脫 水處理之溫度以80〜35(TC較佳。未達80°C時,幾乎無法 進行脫水。超過35(TC時,於繼後之還原處理時,不易在 低溫下製得鐵金屬粒子粉末。更佳的脫水處理溫度爲85 〜3 00〇C。 於脫水處理後,亦可以進行噴射磨、球磨等之粉碎處 理。於此等之處理時,可使用氦氣或氬氣、氮氣等之惰性 氣體。 脫水處理以空氣或氮氣氣體環境較佳。 還原處理溫度爲160〜420°C。還原處理溫度未達 160°C時,鐵化合物粒子粉末無法充分還原成金屬鐵。還 原處理溫度超過420°C時,鐵化合物粒子粉末雖被還原’ 惟由於粒子間進行燒結,氮化率降低。較佳的還原處理溫 度爲165〜380 °C,更佳者爲170〜350 °C。 還原方法沒有特別的限制,可使用氫氣流通、或使用 各種鹵化物化合物之還原方法。 -13- 201249564 還原處理之時間,沒有特別的限制,以1 . 佳。超過24小時時,因還原溫度而不易進行 氮化處理。未達1小時時,大多數無法充分地 者爲1 .5〜1 5小時。 於還原處理後,亦可以噴射磨、球磨等進 。於此等之處理時,可使用氦氣或氬氣、氮氣 體。 於還原處理後,進行氮化處理。 氮化處理的溫度,爲130〜170 °C。氮化處 達130°C時,無法充分地進行氮化處理。氮化There is no particular limitation on the iron oxide or iron oxyhydroxide of the starting material, for example, magnetite, Y-Fe2〇3 ' a-Fe2〇3 ' a-FeOOH ' β-FeOOH -11 - 201249564 , γ-FeOOH, FeO and so on. Further, even if the starting material is a single phase, it may contain impurities, and may contain iron oxide or iron oxyhydroxide other than the main phase as an impurity. The particle shape of the iron oxide or iron oxyhydroxide starting material is not particularly special. The restriction may be any of a needle shape, a granular shape, a spindle shape, a rectangular shape, a spherical shape, and the like. The aspect ratio (long axis diameter / short axis diameter) of the iron compound particle powder of the present invention is preferably 1.0 to 200. When it exceeds this range, it is difficult to obtain a ferromagnetic particle powder composed of a Fe16N2 compound phase of the Mössbauer spectrum of 80% or more. The preferred aspect ratio is from 1.0 to 190, and more preferably from 1.0 to 180. The BET specific surface area of the iron compound particle powder of the starting material is preferably 20 to 25 m 2 /g. When the BET specific surface area is less than 20 m2/g, the nitriding treatment is not easily performed, and the ferromagnetic particle powder composed of the Fe16N2 compound phase of the Mössbauer spectrum of 80% or more cannot be obtained. When the BET specific surface area exceeds 250 m2/g, excessive nitriding is caused, so that a ferromagnetic particle powder composed of a Fe16N2 compound phase of the Mössbauer spectrum of 80% or more cannot be obtained. Preferably, the BET specific surface area is from 30 to 200 m 2 /g, more preferably from 35 to 180 m 2 /g. The agglomerated particle diameter of the iron oxide or iron oxyhydroxide in the starting material of the present invention is controlled to a D50 of 40 μm. Hereinafter, D90 is preferably 150 μm or less. Since the starting material uses a powder, the aggregated particle diameter is generally large. The method of making the aggregated particle diameter small is not particularly limited, and for example, it can be ball milled in the presence of an alcohol compound, a ketone compound, or an organic solvent such as toluene, hexane, carbon tetrachloride, or -12-201249564 cyclohexane. Planetary ball grinding, wet; crushing' and jet milling. Preferably, D50 is 35 μm or less, D90 is 125 μm or less, and more preferably D50 is 30 μm or less, and D90 is 100 μm or less. The iron compound particle powder of the present invention is preferably passed through a sieve of 250 μm or less before heat treatment. When the mesh size exceeds 205 μm, it is difficult to obtain a ferromagnetic particle powder which exhibits desired magnetic properties. Preferably, it is 236 μηι or less. For the iron oxyhydroxide, when the dehydration treatment is required, the temperature of the dehydration treatment is 80 to 35 (TC is preferred. When the temperature is less than 80 ° C, the dehydration is hardly possible. When it exceeds 35 (TC), In the subsequent reduction treatment, it is difficult to obtain the iron metal particle powder at a low temperature. The dehydration treatment temperature is preferably 85 to 300 〇 C. After the dehydration treatment, pulverization treatment such as jet milling or ball milling can also be performed. For such treatment, helium gas or an inert gas such as argon gas or nitrogen gas may be used. The dehydration treatment is preferably carried out in an air or nitrogen gas atmosphere. The reduction treatment temperature is 160 to 420 ° C. When the reduction treatment temperature is less than 160 ° C The iron compound particle powder cannot be sufficiently reduced to metal iron. When the reduction treatment temperature exceeds 420 ° C, the iron compound particle powder is reduced, but the nitridation rate is lowered due to sintering between the particles. The preferred reduction treatment temperature is 165~ 380 ° C, more preferably 170 to 350 ° C. The reduction method is not particularly limited, and hydrogen gas can be used, or a reduction method using various halide compounds can be used. -13- 201249564 Time of reduction treatment, no Other restrictions are better than 1. When it is more than 24 hours, it is not easy to carry out nitriding treatment due to the reduction temperature. When it is less than 1 hour, most of them cannot be fully used for 1.5 to 15 hours. It is also possible to use jet milling, ball milling, etc. For the treatments such as helium or argon or nitrogen gas, the nitriding treatment is carried out after the reduction treatment. The temperature of the nitriding treatment is 130 to 170 °C. When the nitridation reaches 130 ° C, the nitriding treatment cannot be sufficiently performed.
超過”(^時,由於生成γ’-FqN或e-Fe2〜3N 得目的之由穆斯堡爾光譜之Fe16N2化合物相j 所構成的強磁性粒子粉末。較佳的還原溫度爲 〇 氮化處理之時間以5 0小時以內較佳。藉 於工業上生產之短時間完成步驟,以增加每時 工業生產性優異》更佳者爲3 6小時以內。 氮化處理之氣體環境,以NH3氣體環境爲 外亦可使用N2、H2或CH4等之碳化氫氣體、 之中混合過熱水蒸氣等。 氮化處理只要是以上述適當的處理溫度、 時間即可,進行接近1 00%之氮化處理,接 Fe ! 6N2化合物相,即於氮化處理後取出時沒有 氧氣而氧化,在粒子外殻上幾乎完全沒有存在 〜2 4小時較 燒結後段的 還原。更佳 行粉碎處理 等之惰性氣 理之溫度未 處理之溫度 ,故無法製 爲8 0 %以上 135 〜165。。 由儘可能以 間之收a, 宜,除nh3 以及在此等 充分的處理 近 100%之 被空氣中之 FeO,可得 -14 - 201249564A ferromagnetic particle powder consisting of a Fe16N2 compound phase j of the Mössbauer spectrum for the purpose of generating γ'-FqN or e-Fe2~3N. The preferred reduction temperature is ruthenium nitride treatment. The time is preferably within 50 hours. The industrial process is shortly completed in order to increase the industrial productivity per hour. The better is less than 36 hours. The nitriding gas environment is NH3 gas environment. For the outside, a hydrocarbon gas such as N2, H2 or CH4 may be used, and superheated steam may be mixed therein. The nitriding treatment may be carried out by nitriding treatment of approximately 100% as long as the above-mentioned appropriate treatment temperature and time are used. The Fe 6 62 compound phase is oxidized without oxygen when it is taken out after nitriding treatment, and there is almost no 2-4 hours of reduction on the particle shell compared with the post-sintering stage. It is better to perform inert treatment such as pulverization treatment. The temperature is not treated, so it can not be made 80% or more 135 ~ 165. By as much as possible, in addition to nh3 and in this sufficient treatment of nearly 100% of the FeO in the air,得-14 - 20124956 4
Fel6N2化合物相幾乎爲100%之強磁性粒子粉末,惟如上 所述’就工業觀點而言恐無法實現。藉由本發明人等之檢 討’可知以FeI6N2化合物相爲80%以上之比例進行氮化 處理’且即使於氮化處理後存在粒子表面之金屬鐵在空氣 中氧化’導致粒子外殼上產生FeO,只要是FeO膜厚爲 5 nm以下時,不會對強磁性粒子粉末之磁性特性有不良影 響。 因此,沒有必要進行Fe16N2化合物相爲100%之氮化 處理,可進行FeO膜厚約爲5nm以下之氮化處理。例如 ,藉由適當選擇氮化處理時間,亦可調節FeO之膜厚。 其次,說明有關本發明之異向性磁石。 本發明之異向性磁石之磁性特性,可視目的之用途而 定,調整企求的磁性特性(保磁力、殘留磁束密度、最大 能量積)。 予以磁性配向的方法,沒有特別的限制。例如於玻璃 轉移溫度以上之溫度時,在EVA(乙烯-醋酸乙烯酯共聚物 )樹脂中同時混練由穆斯堡爾光譜之Fe16N2化合物相爲 8 0%以上所構成的強磁性粒子粉末與分散劑等予以成形, 在超過玻璃轉移溫度附近之溫度施加企求的外部磁場,可 促進磁性配向。另外,使胺基甲酸酯等之樹脂與有機溶劑 與該強磁性粒子粉末以手動搖動器激烈地進行混合,使經 粉碎的油墨藉由混合或R〇ll-to-R〇ll法予以塗佈印刷於樹 脂薄膜上,且盡快通過磁場中,進行磁性配向。此外,使 用RIP(Resin Isostatic Pressing),進行更高密度且使結晶 -15- 201249564 磁性異向性活用至最大極限的磁性配向。預先在強磁性粒 子粉末中進行二氧化矽或氧化鋁、氧化锆、氧化錫、氧化 銻等之絕緣被覆。絕緣被覆之方法,沒有特別的限制,藉 由控制溶液中之粒子表面電位予以吸附的方法、或以 CVD法等予以蒸鍍。 其次,說明有關本發明之黏結磁石用樹脂組成物》 本發明之黏結磁石用樹脂組成物,係在黏接劑樹脂中 分散本發明之強磁性粒子粉末而成者,由含有85〜99重 量%之該強磁性粒子粉末,且殘餘成分爲黏接劑樹脂與其 他添加劑而成。 亦可預先在強磁性粒子粉末中進行二氧化矽或氧化鋁 、氧化锆、氧化錫、氧化銻等之絕緣被覆。絕緣被覆之方 法,沒有特別的限制,可藉由控制溶液中之粒子表面電位 予以吸附的方法、或以CVD法等予以蒸鍍。 前述黏接劑樹脂,可視成形法而定作各種選擇,爲射 出成形、押出成形及壓延成形時,可使用熱可塑性樹脂, 爲壓縮成形時,可使用熱硬化性樹脂。前述熱可塑性樹脂 ’例如耐龍(PA)系、聚丙烯(PP)系、乙烯醋酸乙烯酯 (EVA)系、聚硫化亞苯基(PPS)系、液晶樹脂(LCP)系、彈 性體系、橡膠系等之樹脂’前述熱硬化性樹脂例如可使用 環氧系、苯酚系等之樹脂。 而且,於製造黏結磁石用樹脂組成物時,爲可容易成 形且可充分發揮磁性特性時’視其所需除黏接劑樹脂外, 亦可添加可塑劑、平滑劑、偶合劑等周知的添加物。而且 -16- 201249564 ,亦可混合純粒鐵磁石粉末等之其他種類的磁石粉末。 此等之添加物,係視目的而定選擇適當即可,可塑劑 可使用視各使用樹脂而定之市售者,其合計量相對於使用 的黏接劑樹脂而言,可使用約0 · 0 1〜5 · 0重量%。 前述平滑劑可使用硬脂酸與其衍生物、無機平滑劑、 油系等,對黏結磁石全體而言可使用約0.01〜1.0重量% 〇 前述偶合劑可使用視使用樹脂與塡充物而定之市售品 ,對使用的黏接劑樹脂而言可使用約0.01〜3.0重量% » 本發明之黏結磁石用樹脂組成物,係使強磁性粒子粉 末與黏接劑樹脂予以混合、混練,製得黏結磁石用樹脂組 成物。 前述混合可以手動混合機、V字型混合機、諾塔 (Nauta)混合機等之混合機進行,混練可以一軸混練機、 二軸混練機、臼型混練機、押出混練機等進行。 其次,說明有關本發明之黏結磁石》 黏結磁石之磁性特性,係視目的之用途而定調整企求 的磁性·特·性·(保磁力、殘留磁束密度、最大能量積)。 本發明之黏結磁石,係可藉由使用前述黏結磁石用樹 脂組成物,以射出成形、押出成形、壓縮成形或壓延成形 等周知的成形法進行成形加工後,以常法進行電磁石著磁 或脈動著磁,形成黏結磁石。 其次,說明有關本發明之燒結磁石。 本發明之燒結磁石,只要是可使強磁性粒子粉末進行 -17- 201249564 壓縮成形及熱處理即可。磁場或壓縮成形的條件,沒有特 別的限制,依照所製作的壓粉磁石之要求値予以調整。例 如,磁場爲1〜15T、壓縮成形壓力爲1.5〜15ton/cm2。 成形機器沒有特別的限制,可使用CIP或RIP。成形體之 形狀或大小符合用途予以選擇。 預先在強磁性粒子粉末中進行二氧化矽或氧化鋁、氧 化鲒、氧化錫、氧化銻等之絕緣被覆。絕緣被覆之方法, 沒有特別的限制,藉由控制溶液中之粒子表面電位予以吸 附的方法、或以CVD法等予以蒸鍍》 平滑劑可使用硬脂酸或其衍生物、無機平滑劑、油系 等,對黏結磁石全體而言,可使用約0.01〜1重量%。 黏著劑可使用聚乙烯、聚丙烯等之聚烯烴類、聚乙烯 醇、聚氧化乙烯、PPS、液晶聚合物、PEEK、聚醯亞胺、 聚醚醯亞胺、聚乙縮醛、聚醚碾、聚颯、聚碳酸酯、聚對 苯二甲酸乙二酯、聚對苯二甲酸丁二酯、聚氧化亞苯基、 聚酞醯胺、聚醯胺等之熱可塑性樹脂或此等之混合物,對 黏結磁石全體而言可使用約0.01〜5.0重量%。 熱處理可適當選擇連續爐或RF高頻率爐等。熱處理 條件沒有特別的限制。 其次,說明有關本發明之壓粉磁石》 本發明之壓粉磁石,係使所得的強磁性粒子粉末在磁 場中進行壓縮成形。磁場或壓縮成形之條件,沒有特別的 限制,依照所製作的壓粉磁石之要求値予以調整。例如, 磁場爲1.0〜15T、壓縮成形壓力爲1.5〜15ton/cm2。成形 -18- 201249564 機器沒有特別的限制,可使用CIP或RIP。成形體之形狀 或大小係符合用途予以選擇。 預先在強磁性粒子粉末中進行二氧化矽或氧化鋁、氧 化鉻、氧化錫、氧化銻等之絕緣被覆。絕緣被覆之方法, 沒有特別的限制,藉由控制溶液中之粒子表面電位予以吸 附的方法、或以CVD法等予以蒸鍍。 平滑劑可使用硬脂酸或其衍生物、無機平滑劑、油系 寺,對黏結磁石全體而3,可使用約0.01〜1重量%。 黏著劑可使用聚乙烯、聚丙烯等之聚烯烴類、聚乙烯 醇、聚氧化乙烯、PPS、液晶聚合物、PEEK、聚醯亞胺、 聚醚醯亞胺、聚乙縮醛、聚醚砸、聚碾、聚碳酸酯、聚對 苯二甲酸乙二酯、聚對苯二甲酸丁二酯、聚氧化亞苯基、 聚酞醯胺、聚醯胺等之熱可塑性樹脂或此等之混合物,對 黏結磁石全體而言可使用約0.01〜5.0重量%。 熱處理可適當選擇連續爐或RF高頻率爐等。熱處理 條件沒有特別的限制。 【實施方式】 本發明典型的實施形態如下所述》 [實施例] 出發原料之氧化鐵或氧基氫氧化鐵或所得的強磁性粒 子粉末之比表面積値,係藉由氮之B.E.T.法進行測定。 出發原料之氧化鐵或氧基氫氧化鐵或所得的強磁性粒 -19- 201249564 子粉末之一次粒子尺寸,係使用透過型電子顯微鏡(曰本 電子(股)' JEM- 1 200EXII)進行測定。計算任意選出的120 個粒子之粒子尺寸,求取其平均値。 出發原料之氧化鐵或氧基氫氧化鐵或所得的強磁性粒 子粉末試料之組成分析,係使經加熱的試料以酸溶解’且 使用電漿發光分光分析裝置(SEIKO電子工業(股)、 SPS4000)進行分析求得》 出發原料及所得的強磁性粒子粉末之構成相,藉由粉 末X光繞射裝置(XRD、Rigaku(股)製、RINT-25 00)同定時 ,進行使用透過型電子顯微鏡(日本電子(股)、JEM-2000EX)、電子線分光型超高分解能電子顯微鏡(HREM、 Hitachi Hitech、HF-2000)之電子線繞射(ED)、電子能量 損失分光法(EELS)、能量分散X光分光法(EDS)、掃描透 過電子顯微鏡(STEM)分析·評估予以決定。藉由ED或 EELS、STEM、EDS之分析.評估,可確認有以XRD無 法得知的作爲雜質相之α-Fe、Fe4N、Fe3-XN、或微量局部 存在經添加的金屬元素X。The Fel6N2 compound phase is almost 100% strong magnetic particle powder, but as described above, it may not be realized from an industrial viewpoint. According to the review by the inventors of the present invention, it is known that the nitriding treatment is carried out at a ratio of 80% or more of the FeI6N2 compound phase, and even if the metal iron having the particle surface is oxidized in the air after the nitriding treatment, the FeO is generated on the particle shell, as long as When the FeO film thickness is 5 nm or less, the magnetic properties of the ferromagnetic particle powder are not adversely affected. Therefore, it is not necessary to carry out a nitriding treatment in which the Fe16N2 compound phase is 100%, and a nitriding treatment in which the FeO film thickness is about 5 nm or less can be performed. For example, the film thickness of FeO can also be adjusted by appropriately selecting the nitriding treatment time. Next, an anisotropic magnet relating to the present invention will be described. The magnetic properties of the anisotropic magnet of the present invention can be adjusted depending on the intended purpose, and the desired magnetic properties (magnetic coercive force, residual magnetic flux density, and maximum energy product) can be adjusted. There is no particular limitation on the method of magnetic alignment. For example, at a temperature higher than the glass transition temperature, a ferromagnetic particle powder and a dispersant composed of a Fe16N2 compound phase of a Mossbauer spectrum of 80% or more are simultaneously kneaded in an EVA (ethylene-vinyl acetate copolymer) resin. When it is formed, an external magnetic field is applied at a temperature exceeding the glass transition temperature to promote magnetic alignment. Further, a resin such as a urethane and an organic solvent are vigorously mixed with the ferromagnetic particle powder by a manual shaker, and the pulverized ink is applied by mixing or R〇ll-to-R〇ll method. The cloth is printed on the resin film and magnetically aligned as soon as possible through a magnetic field. Further, RIP (Resin Isostatic Pressing) was used to carry out magnetic alignment at a higher density and to make the crystal -15-201249564 magnetic anisotropy to the maximum limit. Insulating coating of cerium oxide or aluminum oxide, zirconium oxide, tin oxide, antimony oxide or the like is carried out in advance in the ferromagnetic particle powder. The method of insulating coating is not particularly limited, and it is deposited by controlling the surface potential of the particles in the solution or by vapor deposition by a CVD method or the like. Next, the resin composition for a bonded magnet according to the present invention will be described. The resin composition for a bonded magnet of the present invention is obtained by dispersing the ferromagnetic particle powder of the present invention in an adhesive resin, and contains 85 to 99% by weight. The ferromagnetic particle powder is obtained, and the residual component is an adhesive resin and other additives. Insulating coating of cerium oxide or aluminum oxide, zirconium oxide, tin oxide, cerium oxide or the like may be carried out in advance in the ferromagnetic particle powder. The method of insulating coating is not particularly limited, and it can be deposited by a method of controlling the surface potential of the particles in the solution or by a CVD method or the like. The above-mentioned adhesive resin can be variously selected depending on the molding method, and a thermoplastic resin can be used for injection molding, extrusion molding, and calender molding, and a thermosetting resin can be used for compression molding. The thermoplastic resin is, for example, Nylon (PA), polypropylene (PP), ethylene vinyl acetate (EVA), polysulfide (PPS), liquid crystal resin (LCP), elastic system, rubber Resin of the system, etc. As the thermosetting resin, for example, an epoxy resin or a phenol resin can be used. Further, in the case of producing a resin composition for a bonded magnet, in order to facilitate molding and to sufficiently exhibit magnetic properties, a known plasticizer, a smoothing agent, a coupling agent, or the like may be added in addition to the adhesive resin required. Things. Further, -16-201249564, other types of magnet powder such as pure ferromagnetic powder may be mixed. These additives may be appropriately selected depending on the purpose, and the plasticizer may be used as a commercial product depending on the resin to be used, and the total amount thereof may be about 0. 0 with respect to the adhesive resin to be used. 1 to 5 · 0% by weight. As the smoothing agent, stearic acid and a derivative thereof, an inorganic smoothing agent, an oil system, or the like can be used, and about 0.01 to 1.0% by weight can be used for the entire bonded magnet. The coupling agent can be used depending on the resin and the filling. For the adhesive resin to be used, about 0.01 to 3.0% by weight can be used. » The resin composition for a bonded magnet of the present invention is obtained by mixing and kneading a ferromagnetic particle powder and a binder resin to obtain a bond. A resin composition for magnets. The mixing may be carried out by a mixer such as a hand mixer, a V-shaped mixer or a Nauta mixer, and the kneading may be carried out by a one-axis kneading machine, a two-axis kneading machine, a kneading type kneading machine, an extrusion kneading machine or the like. Next, the magnetic properties of the bonded magnet of the present invention will be described. The magnetic properties, the magnetic properties, the residual magnetic flux density, and the maximum energy product are adjusted depending on the intended use. The bonded magnet of the present invention can be formed by a known molding method such as injection molding, extrusion molding, compression molding or calender molding by using the resin composition for a bonded magnet, and then magnetizing or pulsing the electromagnet by a usual method. Magnetically, forming a bonded magnet. Next, a sintered magnet relating to the present invention will be described. The sintered magnet of the present invention may be subjected to compression molding and heat treatment of the ferromagnetic particle powder at -17 to 201249564. The conditions of the magnetic field or compression molding are not particularly limited and are adjusted in accordance with the requirements of the pressed powder magnet. For example, the magnetic field is 1 to 15 T and the compression molding pressure is 1.5 to 15 ton/cm 2 . The forming machine is not particularly limited, and CIP or RIP can be used. The shape or size of the shaped body is selected according to the use. An insulating coating of cerium oxide or aluminum oxide, cerium oxide, tin oxide, cerium oxide or the like is carried out in advance in the ferromagnetic particle powder. The method of insulating coating is not particularly limited, and a method of adsorbing the surface potential of the particles in the solution or a method of vapor deposition by a CVD method or the like can be used. Stearic acid or a derivative thereof, an inorganic smoothing agent, and an oil can be used. For example, for the entire bonded magnet, about 0.01 to 1% by weight can be used. As the adhesive, polyolefins such as polyethylene and polypropylene, polyvinyl alcohol, polyethylene oxide, PPS, liquid crystal polymer, PEEK, polyimine, polyether oxime, polyacetal, polyether mill can be used. a thermoplastic resin such as polyfluorene, polycarbonate, polyethylene terephthalate, polybutylene terephthalate, polyoxyphenylene, polydecylamine, polydecylamine or the like or a mixture thereof For the entire bonded magnet, about 0.01 to 5.0% by weight can be used. The heat treatment can be appropriately selected from a continuous furnace or an RF high frequency furnace. The heat treatment conditions are not particularly limited. Next, a description will be given of a dust magnet according to the present invention. The powder magnetic magnet of the present invention is obtained by subjecting the obtained ferromagnetic particle powder to compression molding in a magnetic field. The conditions of the magnetic field or compression molding are not particularly limited, and are adjusted in accordance with the requirements of the produced powder magnet. For example, the magnetic field is 1.0 to 15 T and the compression molding pressure is 1.5 to 15 ton/cm 2 . Forming -18- 201249564 There are no special restrictions on the machine. CIP or RIP can be used. The shape or size of the shaped body is selected according to the application. An insulating coating of cerium oxide or aluminum oxide, chromium oxide, tin oxide, cerium oxide or the like is carried out in advance in the ferromagnetic particle powder. The method of insulating coating is not particularly limited, and it is deposited by controlling the surface potential of the particles in the solution or by vapor deposition by a CVD method or the like. As the smoothing agent, stearic acid or a derivative thereof, an inorganic smoothing agent, or an oil-based temple can be used, and the total amount of the bonded magnets can be 3, and about 0.01 to 1% by weight can be used. As the adhesive, polyolefins such as polyethylene and polypropylene, polyvinyl alcohol, polyethylene oxide, PPS, liquid crystal polymer, PEEK, polyimine, polyether oxime, polyacetal, polyether oxime can be used. , thermoplastic, polycarbonate, polyethylene terephthalate, polybutylene terephthalate, polyoxyphenylene, polydecylamine, polydecylamine, etc., or a mixture thereof For the entire bonded magnet, about 0.01 to 5.0% by weight can be used. The heat treatment can be appropriately selected from a continuous furnace or an RF high frequency furnace. The heat treatment conditions are not particularly limited. [Embodiment] A typical embodiment of the present invention is as follows: [Examples] The specific surface area 値 of iron oxide or iron oxyhydroxide of the starting material or the obtained ferromagnetic particle powder is determined by a nitrogen BET method. . The primary particle size of the starting material of iron oxide or iron oxyhydroxide or the obtained ferromagnetic particles -19-201249564 sub-powder was measured using a transmission electron microscope (Sakamoto Electronics Co., Ltd. JEM-1200EXII). Calculate the particle size of any selected 120 particles and find the average 値. The composition analysis of the iron oxide or iron oxyhydroxide powder of the starting material or the obtained ferromagnetic particle powder sample is such that the heated sample is dissolved in acid' and the plasma luminescence spectroscopic analyzer is used (SEIKO Electronics Industry Co., Ltd., SPS4000) The analysis was carried out to obtain the constituent phase of the starting material and the obtained ferromagnetic particle powder, and the powder X-ray diffraction apparatus (XRD, Rigaku Co., Ltd., RINT-25 00) was used at the same timing to carry out the transmission electron microscope. (Japan Electronics Co., Ltd., JEM-2000EX), Electron Line Diffraction (ED), Electron Energy Loss Spectrometry (EELS), Energy for Electron Beam Spectroscopic Ultra High Decomposition Energy Electron Microscope (HREM, Hitachi Hitech, HF-2000) Dispersive X-ray spectroscopy (EDS), scanning electron microscopy (STEM) analysis and evaluation were determined. By analysis of ED or EELS, STEM, and EDS, it was confirmed that α-Fe, Fe4N, Fe3-XN, or a trace amount of the added metal element X which is not known as an impurity phase by XRD.
FeO之體積分率係如下述進行評估。 首先,有關強磁性粒子粉末係使用電子能量損失分光 法(EELS),確認FeO(氧)之存在位置。然後,於強磁性粒 子粉末之TEM觀察時,可確認粒子之中心部與對比不同 的部分,且以前述電子能量損失分光法(EELS)之結果爲基 準,確認FeO之存在位置,測定FeO之厚度,且由FeO 之厚度與粒子形狀求得FeO之體積分率。 -20- 201249564 所得的強磁性粒子粉末之格子定數,係使用粉末χ 光繞射裝置(XRD、Rigaku(股)製、RINT-2500)求得。該格 子定數參照原有的下述文獻,求取氮量。 (#考文獻) •高橋有紀子 東北大學大學院工學硏究科電子工學專攻 200 1 年博士學位論文題目: 「有關(C,N)添加Fe基合金薄膜 之非平衡α’、α” ' γ相之合成與磁性的硏究」 • K.H. Jack, P r 〇 c . Roy. Soc.,A2 0 8, 216(1951) “The iron-nitrogen system : the preparation and the crystal structures of nitro gen-austenite (γ) and nitrogen-martensite(a,)’’ 所得的強磁性粒子粉末之磁氣特性,係使用物理特性 測定系統(PPMS + VSM、Japan Quantum· Design(股)),在 室溫(3 0 0K)下、0〜9T之磁場中進行測定。另外,亦進行 評估5K〜300K爲止之磁化率的溫度相關性。 所得的強磁性粒子粉末之穆斯堡爾測定,係在氬氣氣 體環境之套手工具箱中,使強磁性粒子粉末與矽油脂更均 勻地混合,包於鋁孔中,於液體中在氦氣溫度至室溫之範 圍內進行3〜4日,再藉由分析數據,求取所得的強磁性 粒子粉末Fe16N2的生成比例。進行檢討ct-Fe、Fe4N、 Fe3_xN、或氧化鐵等之副成分作爲分析時之雜質相。 -21 - 201249564 出發原料之粒度分布測定,溶劑係使用純水,藉由 Malvern 製、Mastersizer 20 00E 進行測定。 實施例1 : <出發原料之調製> 使用硫酸亞鐵、苛性鹼、碳酸鈉製作平均長軸直徑 2 10nm、縱橫軸比7、比表面積n8rn2/g之紡錘狀針鐵礦 粒子。以努採漏斗(Nutsche)過濾分離該物,對試料5g而 言’以相當純水150ml之純水進行洗淨。然後,以13(TC 之通風乾燥機進行乾燥1晚。 <出發原料之粉碎處理> 其次,在己烷溶劑35ml中加熱乾燥粉末試料3g, 同時以之氮化矽珠與以氮氣取代之行星球磨、在 室溫下進行粉碎4小時,再取出粉末。進行該粉末之粒度 分布測定時,D50爲1.6μιη、D90爲4.4μιη。 <出發原料之還原處理及氮化處理> 重複進行數次與上述相同的處理,使用出發原料後, 以振動篩僅萃取90μπι以下之凝聚粒子之試料粉末5〇g, 加入氧化銘製甲跡(125mm><125mmx深度30mm),靜置於 熱處理爐中。將爐內抽成真空後,塡充氬氣,再重複3次 抽成真空的操作《•然後,使氫氣以5L/min之流量流通, 且以5°C/min之昇溫速度昇溫至27 7t且保持3小時,進 -22- 201249564 行還原處理。然後,降溫至152°C ’停止供應氫氣。而且 ,以該狀態取出的試料’以α-Fe單相之比表面積爲 19.5m2/g。繼後,使銨氣與氮氣與氫氣之混合比例爲9: 0.95 : 0.15之混合氣體以全量流入.l〇L/min,且在148°C 下進行氮化處理7小時。然後’流通氬氣,降溫至室溫, 且停止供應氬氣,進行空氣取代3小時。 <所得的試料之分析.評估> 所得的粒子粉末,藉由XRD、ED爲Fe16N2,藉由穆 斯堡爾光譜測定,Fe16N2化合物相爲91‘%。平均長軸直徑 195nm、比表面積19.7m2/g、FeO膜厚爲3nm、FeO之體 積分率爲24.6%。而且,氮化率爲8.9%。測定磁性特性時 ’以5K之飽和磁化値os = 238emu/g,保磁力H(; = 2.1kOe» 實施例2 : 與實施例1相同地,使用硫酸亞鐵、苛性鹼、碳酸鈉 製作平均長軸直徑665nm、縱橫軸比19、比表面積 67m2/g之紡錘狀針鐵礦粒子。以努採漏斗過濾分離該物 ’相對於試料5g而言,以相當純水150ml之純水進行洗 淨。然後’以1 25 °C之通風乾燥機進行乾燥1晚。另外, 以噴霧式粉碎機與振動篩僅萃取250μιη以下之凝聚粒子 °達行測定該粉末之粒度分布時,D50爲17.1μιη、D90爲 4 6,0 μηι。 其次,與實施例1相同地進行還原處理與氮化處理。 -23- 201249564 還原處理係在2 8 8 t下進行2 · 5小時。而且,以該狀態取 出的試料,α-Fe單相之比表面積爲9.3m2/g。氮化處理係 使銨氣以10L/min流通且在152°C下進行氮化處理4小時 〇 所得的粒子粉末,藉由XRD、ED爲Fel6N2,藉由穆 斯堡爾光譜測定,Fe16N2化合物相爲93%。而且,平均長 軸直徑630nm、比表面積9.4m2/g、FeO膜厚爲2nm、FeO 之體積分率爲8.6%。而且,氮化率爲9.4%。測定磁性特 性時,以 5K之飽和磁化値 as = 226emu/g,保磁力 Hc= 1.9kOe。 實施例3 : 以Fe元素換算0.96: 2稱取硫酸鐵與硫酸亞鐵,藉 由在較苛性鈉更高的鹼狀態下進行反應,製作平均長軸直 徑50nm、縱橫軸比1.01、比表面積92m2/g之立方體狀磁 鐵礦粒子。以努採漏斗過濾分離該物,相對於試料5g而 言,以相當純水 200ml之純水進行洗淨。然後,以6〇〇c 之通風乾燥機進行乾燥1.5日。使該物在甲苯溶劑中使用 15wt%固成分濃度、5 00μιη之氮化矽製珠進行濕式珠磨粉 碎。進行測定該粉末之粒度分布時,D50爲8.8μιη、D90 爲15.2μπι。另外’以振動篩僅萃取ι80μΓη以下之凝聚粒 子。此外’與實施例2相同地進行還原處理與氮化處理。 而且,以還原處理後之狀態所取出的試料,a_Fe單相之 比表面積爲38.0m2/g。 -24- 201249564 所得的粒子粉末,藉由XRD、ED爲Fei6N2 ’藉由穆 斯堡爾光譜測定,Fe16N2化合物相爲85%。而且,平均長 軸直徑42nm、比表面積38.2m2/g、FeO膜厚爲1.5nm、 FeO之體積分率爲13.8%、氮化率爲11.8%。測定磁性特 性時,飽和磁化値as=198emu/g ’保磁力Hc=l .7kOe。 實施例4 : 在苛性鈉與碳酸鈉之混合溶液中加入有氯化鐵、檸檬 酸鈉之混合溶液中,使空氣起泡,製作平均長軸直徑 2 5 00nm、縱橫軸比45.5、比表面積85.9m2/g之針狀纖鐵 礦粒子。以努採漏斗過濾分離該物,相對於試料5g而言 ,以相當純水 200ml之純水進行洗淨。然後,在120°C下 進行乾燥1晚,再繼續於3 5 0°C下進行熱處理1小時。於 噴霧式粉碎機後,與實施例3相同地以濕式珠磨進行粉碎 處理。進行測定該粉末之粒度分布時,D50爲5.4μιη、 D90爲13·9μηι。另外’以振動篩僅萃取ΐ80μιη以下之凝 聚粒子。此外,與實施例2相同地進行還原處理與氮化處 理。還原係在氫氣氣流中、220 °C下進行8 ..小時,氮化處 理係在銨氣氣流中、1 4 8 °C下各進行1 4小時。而且,以還 原處理後之狀態取出的試料,爲α _ F e單相 '比表面積爲 1 4.3 m2/g。 所得的粒子粉末’藉由XRD、ED爲Fe16N2,藉由穆 斯堡爾光譜測定’ F e ! 2化合物相爲8 7 %。而且,平均長 軸 ΐΐί 徑 2450nm、比表面積 i4.6m2/g、FeO 膜厚爲 2.3nm、 -25- 201249564The volume fraction of FeO was evaluated as follows. First, regarding the ferromagnetic particle powder, the position of FeO (oxygen) was confirmed by electron energy loss spectroscopy (EELS). Then, in the TEM observation of the ferromagnetic particle powder, it was confirmed that the center portion of the particle was different from the contrast, and the position of FeO was confirmed based on the result of the electron energy loss spectrometry (EELS), and the thickness of FeO was measured. And the volume fraction of FeO is determined from the thickness of FeO and the shape of the particles. -20- 201249564 The lattice constant of the obtained ferromagnetic particle powder was determined using a powder calender diffraction apparatus (XRD, manufactured by Rigaku Co., Ltd., RINT-2500). The grid number is determined by referring to the following literature to determine the amount of nitrogen. (#Certificate) • Takahashi Yoshiko Tohoku University Graduate School of Engineering, Department of Electrical Engineering, 2001, PhD thesis title: "About (C, N) Adding Fe-based alloy film unbalanced α', α" ' KH Jack, P r 〇c . Roy. Soc., A2 0 8, 216 (1951) “The iron-nitrogen system : the preparation and the crystal structures of nitro gen-austenite (γ) and nitrogen-martensite(a,)'' The magnetic properties of the obtained ferromagnetic particle powder are measured using a physical property measurement system (PPMS + VSM, Japan Quantum·Design) at room temperature (3 0 0K) measured in a magnetic field of 0 to 9 T. The temperature dependence of the magnetic susceptibility of 5 K to 300 K was also evaluated. The Mössbauer measurement of the obtained ferromagnetic particle powder was performed in an argon gas atmosphere. In the kit, the ferromagnetic particle powder is more uniformly mixed with the strontium fat, wrapped in an aluminum hole, and carried out in the liquid at a temperature ranging from xenon to room temperature for 3 to 4 days, and then analyzed by data. Obtaining the obtained ferromagnetic particle powder Proportion of Fe16N2. Review the secondary components such as ct-Fe, Fe4N, Fe3_xN, or iron oxide as the impurity phase during analysis. -21 - 201249564 Determination of particle size distribution of starting materials, solvent using pure water, by Malvern The measurement was carried out by Mastersizer 20 00E. Example 1: <Preparation of starting materials> A spindle shape having an average major axis diameter of 2 10 nm, a medial torse axis ratio of 7, and a specific surface area of n8 rn 2 /g was produced using ferrous sulfate, caustic soda or sodium carbonate. The goethite particles were separated by filtration through a Nutsche funnel (Nutsche), and washed with pure water of 150 ml of pure water for 5 g of the sample, and then dried for 1 night at 13 (TC ventilator). <Pulverization treatment of starting raw material> Next, 3 g of the powder sample was dried by heating in 35 ml of a hexane solvent, and the ruthenium nitride beads and the planetary ball mill substituted with nitrogen were pulverized at room temperature for 4 hours, and then the powder was taken out. When the particle size distribution measurement of the powder is carried out, D50 is 1.6 μm and D90 is 4.4 μm. <Reduction treatment and nitriding treatment of starting materials> The same treatment as above is repeated several times, and the same treatment is used. After the starting material to the vibrating screen only 90μπι extracted sample powder of agglomerated particles of 5〇g oxide was added Ming A track system (125mm > < 125mmx depth 30mm), to stand in a heat treatment furnace. After evacuating the furnace, the argon gas is filled, and the vacuum is repeated three times. "• Then, the hydrogen gas is circulated at a flow rate of 5 L/min, and the temperature is raised to 27 7 t at a temperature increase rate of 5 ° C/min. And keep it for 3 hours, go into the -22-201249564 line to restore. Then, the temperature was lowered to 152 ° C ' to stop the supply of hydrogen. Further, the sample taken out in this state had a specific surface area of α-Fe single phase of 19.5 m 2 /g. Subsequently, a mixed gas of ammonium gas and nitrogen gas and hydrogen gas was mixed at a ratio of 9:0.95 : 0.15 in a total amount of .l 〇L/min, and nitriding treatment was performed at 148 ° C for 7 hours. Then, argon gas was passed through, the temperature was lowered to room temperature, and the supply of argon gas was stopped, and air substitution was carried out for 3 hours. <Analysis of the obtained sample. Evaluation> The obtained particle powder was determined by Mossbauer spectroscopy by XRD and ED as Fe16N2, and the Fe16N2 compound phase was 91%. The average major axis diameter was 195 nm, the specific surface area was 19.7 m2/g, the FeO film thickness was 3 nm, and the volume integral ratio of FeO was 24.6%. Moreover, the nitridation rate was 8.9%. When the magnetic properties were measured, 'saturation magnetization at 5 K 値 os = 238 emu/g, coercive force H (; = 2.1 kOe» Example 2: Same as Example 1, using ferrous sulfate, caustic soda, sodium carbonate to make an average length Spindle-like goethite particles having a shaft diameter of 665 nm, a medial aspect ratio of 19, and a specific surface area of 67 m 2 /g. The product was separated by filtration under a Nou funnel, and washed with pure water of 150 ml of pure water. Then, it was dried for 1 night at a ventilator at 1 25 ° C. In addition, when the particle size distribution of the powder was measured by extracting only agglomerated particles of 250 μm or less with a spray mill and a vibrating screen, the D50 was 17.1 μm, D90. The reduction treatment and the nitridation treatment were carried out in the same manner as in Example 1. -23- 201249564 The reduction treatment was carried out at 2 8 8 t for 2 hours, and the sample taken out in this state was taken. The specific surface area of α-Fe single phase is 9.3 m 2 /g. The nitriding treatment is a particle powder obtained by circulating ammonium gas at 10 L/min and nitriding at 152 ° C for 4 hours, by XRD, ED. Fe16N2 compound as determined by Mossbauer spectrometry for Fel6N2 The average major axis diameter is 630 nm, the specific surface area is 9.4 m 2 /g, the FeO film thickness is 2 nm, and the volume fraction of FeO is 8.6%. Moreover, the nitridation rate is 9.4%. When the magnetic properties are measured, 5K is measured. The saturation magnetization 値 as = 226emu / g, coercive force Hc = 1.9kOe. Example 3: 0.96: 2 in terms of Fe element: 2 ferric sulphate and ferrous sulphate were weighed, in a base state higher than caustic sodium The reaction was carried out to prepare cubic magnetite particles having an average major axis diameter of 50 nm, a medial to lateral axis ratio of 1.01, and a specific surface area of 92 m 2 /g. The material was separated by filtration using a Nou funnel, and was purified to a purity of 200 ml with respect to 5 g of the sample. The water was washed, and then dried for 1.5 days in a 6 m air dryer. The material was wet-bead milled in a toluene solvent using a 15 wt% solid content concentration and 500 μm of a tantalum nitride bead. When the particle size distribution of the powder was measured, the D50 was 8.8 μm and the D90 was 15.2 μm. Further, only the aggregated particles of ι 80 μΓη or less were extracted by a vibrating sieve. Further, the reduction treatment and the nitriding treatment were carried out in the same manner as in Example 2. In the state after the restoration process The sample had a specific surface area of a_Fe single phase of 38.0 m 2 /g. -24 - 201249564 The obtained particle powder was determined by Mossbauer spectroscopy by XRD and ED as Fe6N2 ', and the Fe16N2 compound phase was 85%. The average major axis diameter was 42 nm, the specific surface area was 38.2 m 2 /g, the FeO film thickness was 1.5 nm, the FeO volume fraction was 13.8%, and the nitridation ratio was 11.8%. When the magnetic properties were measured, the saturation magnetization 値 as = 198 emu / g ' coercive force Hc = 1.7 kOe. Example 4: A mixed solution of ferric chloride and sodium citrate was added to a mixed solution of caustic soda and sodium carbonate to foam air, and an average major axis diameter of 2 500 nm, a longitudinal axis ratio of 45.5, and a specific surface area of 85.9 were prepared. Needle-shaped fibrite particles of m2/g. This material was separated by filtration through a Buchner funnel, and washed with purified water of 200 ml of pure water with respect to 5 g of the sample. Then, drying was carried out at 120 ° C for 1 night, and further heat treatment was continued at 350 ° C for 1 hour. After the spray mill, the pulverization treatment was carried out by wet bead milling in the same manner as in the third embodiment. When the particle size distribution of the powder was measured, D50 was 5.4 μm and D90 was 13·9 μη. Further, only the aggregated particles of ΐ80 μm or less were extracted by a vibrating sieve. Further, reduction treatment and nitridation treatment were carried out in the same manner as in Example 2. The reduction was carried out in a hydrogen gas stream at 220 ° C for 8 hours, and the nitridation treatment was carried out in an ammonium gas stream at 14 8 ° C for 14 hours. Further, the sample taken out in the state after the reduction treatment was α _ F e single phase 'specific surface area was 1 4.3 m 2 /g. The obtained particle powder ' was determined by Mossbauer spectroscopy by XRD and ED as Fe16N2, and the compound phase of the F e ! 2 compound was 87%. Moreover, the average long axis ΐΐί diameter is 2450 nm, the specific surface area is i4.6 m2/g, and the FeO film thickness is 2.3 nm, -25- 201249564
FeO之體積分率爲9·4%、氮化率爲10.5%。測定磁性特性 時,飽和磁化値as = 223emu/g,保磁力He = 2.5kOe。 比較例1 : 與實施例1相同地,使用氯化亞鐵、苛性鹼、碳酸鈉 製作平均長軸直徑18〇nm、縱橫軸比6.4、比表面積 1 27m2/g之紡錘狀針鐵礦粒子。以努採漏斗過濾分離該物 ,相對於試料5 g而言,以相當純水 1 5 0 m 1之純水進行洗 淨。然後,以130°C之通風乾燥機進行乾燥1晚。然後, 以氧化鋁乳缽進行粉碎3分鐘,製得D50爲63μιη、D90 爲1 24μπι之粉末試料。 其次,與實施例1相同地進行還原處理與氮化處理。 還原處理係在30(TC下進行2.5小時。而且,以該狀態取 出的試料,爲α-Fe單相、比表面積爲16.2m2/g。氮化處 理係使銨氣以10L/min流通且在158°C下進行氮化處理11 小時。於氮化處理後,在室溫下使爐內以氮氣取代且直接 取出於爐外。 所得的粒子粉末,藉由XRD、ED混合存在有Fe16N2 、Fe4N、α-Fe,藉由穆斯堡爾光譜測定,Fe16N2化合物相 爲79%。而且,平均長軸直徑I60nm、比表面積16.5m2/g ' FeO膜厚爲5.5nm、FeO之體積分率爲53.4%。而且, 氮化率爲7·3%。測定磁性特性時,以5K之飽和磁化値 as=178emu/g,保磁力 He = 1.2kOe。 -26-The volume fraction of FeO was 9.4% and the nitridation rate was 10.5%. When the magnetic properties were measured, the saturation magnetization 値 as = 223 emu/g and the coercive force He = 2.5 kOe. Comparative Example 1: In the same manner as in Example 1, spindle-shaped goethite particles having an average major axis diameter of 18 〇 nm, a medial and lateral axis ratio of 6.4, and a specific surface area of 1,27 m 2 /g were produced using ferrous chloride, caustic soda or sodium carbonate. The material was separated by filtration through a nucleus funnel, and washed with purified water of a relatively pure water of 550 m1 with respect to 5 g of the sample. Then, it was dried overnight at 130 ° C in a ventilator. Then, the powder was pulverized in an alumina mortar for 3 minutes to prepare a powder sample having a D50 of 63 μm and a D90 of 1 24 μm. Next, reduction treatment and nitridation treatment were carried out in the same manner as in Example 1. The reduction treatment was carried out at 30 (TC) for 2.5 hours. Further, the sample taken out in this state was α-Fe single phase and had a specific surface area of 16.2 m 2 /g. The nitriding treatment was carried out by circulating ammonium gas at 10 L/min. The nitriding treatment was carried out for 11 hours at 158 ° C. After the nitriding treatment, the furnace was replaced with nitrogen at room temperature and directly taken out of the furnace. The obtained particle powder was mixed with X16 and ED in the presence of Fe16N2 and Fe4N. , α-Fe, Fe16N2 compound phase is 79% by Mossbauer spectroscopy, and the average major axis diameter is I60nm, specific surface area is 16.5m2/g 'FeO film thickness is 5.5nm, and FeO volume fraction is 53.4. %, and the nitridation rate is 7.3%. When the magnetic properties are measured, the saturation magnetization of 5K is 178as=178emu/g, and the coercive force is He = 1.2kOe.
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